Search results for "particle detector"

showing 10 items of 200 documents

JEM–X: The X-ray monitor aboard INTEGRAL

2003

The JEM-X monitor provides X-ray spectra and imaging with arcminute angular resolution in the 3 to 35 keV band. The good angular resolution and the low energy response of JEM-X plays an important role in the identification of gamma ray sources and in the analysis and scientific interpretation of the combined X-ray and gamma ray data. JEM-X is a coded aperture instrument consisting of two identical, coaligned telescopes. Each of the detectors has a sensitive area of 500 cm 2 , and views the sky through its own coded aperture mask. The two coded masks are inverted with respect to each other and provides an angular resolution of 3 0 across an eective field of view of about 10 diameter.

PhysicsInstrumentation: detectors; X-rays: general;010504 meteorology & atmospheric sciencesSpectrometerbusiness.industryAstrophysics::High Energy Astrophysical PhenomenaResolution (electron density)Astrophysics::Instrumentation and Methods for AstrophysicsGamma rayAstronomy and AstrophysicsField of viewCosmic rayAstrophysics01 natural sciencesParticle detectorOpticsSpace and Planetary Science0103 physical sciencesAngular resolutionCoded aperturebusiness010303 astronomy & astrophysics0105 earth and related environmental sciencesAstronomy & Astrophysics
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Mono-energetic electron induced single-event effects at the VESPER facility

2016

We present experimental evidence of electron induced upsets in a reference ESA SEU monitor, the SEU based particle detector, induced by 200 MeV electron beam at the VESPER facility at CERN. Comparison of experimental cross sections and simulated cross sections are shown and the differences are analyzed. Possible secondary contributions to the upset rate by neutrons and cumulative dose effects are discussed, showing that electronuclear reactions are the expected SEU mechanism. Insight is given as to possible overall electron contribution to the upset rates in the Jovian radiation environment inside a typical spacecraft shielding are evaluated.

PhysicsLarge Hadron Collider010308 nuclear & particles physicsElectronRadiation01 natural sciencesUpsetParticle detectorNuclear physics0103 physical sciencesElectromagnetic shieldingCathode rayNeutron010306 general physics2016 16th European Conference on Radiation and Its Effects on Components and Systems (RADECS)
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The LHCf detector at the CERN Large Hadron Collider

2008

LHCf is an experiment dedicated to the measurement of neutral particles emitted in the very forward region of LHC collisions. The physics goal is to provide data for calibrating the hadron interaction models that are used in the study of Extremely High-Energy Cosmic-Rays. This is possible since the laboratory equivalent collision energy of LHC is 10(17) eV. Two LHCf detectors, consisting of imaging calorimeters made of tungsten plates, plastic scintillator and position sensitive sensors, are installed at zero degree collision angle +/- 140m from an interaction point (IP). Although the lateral dimensions of these calorimeters are very compact, ranging from 20 mm x 20 mm to 40 mm x 40 mm, the…

PhysicsLarge Hadron ColliderLuminosity (scattering theory)Interaction pointPhysics::Instrumentation and Detectorsbusiness.industryDetectorFísicaCosmic rayScintillatorParticle detectorOpticsMeasuring instrumentHigh Energy Physics::ExperimentDetectors and Experimental TechniquesbusinessInstrumentationMathematical PhysicsJournal of Instrumentation
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New information on 12C states from the decays of 12N and 12B

2003

Abstract The properties of states in 12 C above the 3α-threshold are of high current interest for nuclear astrophysics and for the nuclear many-body problem in general. We have initiated a series of experiments aimed at elucidating this region by using the β-decays of 12 N and 12 B. By applying the ISOL method for producing these radioactive isotopes, in combination with modern segmented charged particle detectors, our approach has significant advantages over previous studies of this region.

PhysicsMany-body problemNuclear physicsNuclear and High Energy PhysicsParticle physicsIsotopeNuclear astrophysicsNuclear structureCarbon-12Nuclear ExperimentIsotopes of berylliumRadioactive decayParticle detectorNuclear Physics A
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Performance of the large scale HV-CMOS pixel sensor MuPix8

2019

The Mu3e experiment is searching for the charged lepton flavour violating decay $ ��^+\rightarrow e^+ e^- e^+ $, aiming for an ultimate sensitivity of one in $10^{16}$ decays. In an environment of up to $10^9$ muon decays per second the detector needs to provide precise vertex, time and momentum information to suppress accidental and physics background. The detector consists of cylindrical layers of $50\, ��\text{m}$ thin High Voltage Monolithic Active Pixel Sensors (HV-MAPS) placed in a $1\,\text{T}$ magnetic field. The measurement of the trajectories of the decay particles allows for a precise vertex and momentum reconstruction. Additional layers of fast scintillating fibre and tile detec…

PhysicsMuonPhysics - Instrumentation and Detectors010308 nuclear & particles physicsbusiness.industryPhysics::Instrumentation and DetectorsDetectorFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)01 natural sciencesParticle detector030218 nuclear medicine & medical imagingSemiconductor detectorMomentum03 medical and health sciencesParticle decay0302 clinical medicineOpticsCMOS0103 physical sciencesHigh Energy Physics::ExperimentbusinessInstrumentationMathematical PhysicsLepton
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A polarized 3He target for the photon beam at MAMI

2011

Abstract A polarized 3 He target has been installed for the first time inside the 4 π Crystal Ball detector at the tagged photon beam of the MAinz MIcrotron (MAMI). It has been demonstrated that the system works reliably and that the polarization losses during handling of the polarized gas are under control. Initial polarization values up to 70% and total relaxation times up to 20 h could be obtained during a first test beam time devoted to the measurement of the double polarized photoabsorption cross-section in the Δ ( 1232 ) baryon resonance region.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsDetectorPolarization (waves)01 natural sciencesParticle detectorDelta baryonNuclear physicsBaryonHelium-30103 physical sciencesPhysics::Accelerator Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Atomic physics010306 general physicsNuclear ExperimentInstrumentationMicrotronCrystal Ball
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Real-time calibration of the A4 electromagnetic lead fluoride (PbF2) calorimeter

2011

Abstract Sufficient energy resolution is the key issue for the calorimetry in particle and nuclear physics. The calorimeter of the A4 parity violation experiment at MAMI is a segmented calorimeter where the energy of an event is determined by summing the signals of neighboring channels. In this case, the precise matching of the individual modules is crucial to obtain a good energy resolution. We have developed a calibration procedure for our total absorbing electromagnetic calorimeter which consists of 1022 lead fluoride (PbF 2 ) crystals. This procedure reconstructs the single-module contributions to the events by solving a linear system of equations, involving the inversion of a 1022×1022…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsLead fluorideCalorimetry[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]System of linear equations7. Clean energy01 natural sciencesParticle detectorComputational physicsCalorimeterNuclear physicsElectromagnetic calorimeter0103 physical sciencesMeasuring instrument010306 general physicsInstrumentationBeam (structure)
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Silicon as an Unconventional Detector in Positron Emission Tomography.

2012

Positron emission tomography (PET) is a widely used technique in medical imaging and in studying small animal models of human disease. In the conventional approach, the 511 keV annihilation photons emitted from a patient or small animal are detected by a ring of scintillators such as LYSO read out by arrays of photodetectors. Although this has been a successful in achieving ~5mm FWHM spatial resolution in human studies and ~1mm resolution in dedicated small animal instruments, there is interest in significantly improving these figures. Silicon, although its stopping power is modest for 511 keV photons, offers a number of potential advantages over more conventional approaches. Foremost is it…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsbusiness.industryPhysics::Instrumentation and DetectorsDetectorPhysics::Medical PhysicsPhotodetectorScintillator01 natural sciencesParticle detectorLyso-Article030218 nuclear medicine & medical imagingSemiconductor detector03 medical and health sciences0302 clinical medicineOptics0103 physical sciencesMedical imagingbusinessInstrumentationImage resolutionNuclear instrumentsmethods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment
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Cosmic ray physics with the ALEPH detector

2000

Abstract ALEPH is one of the four detectors at the Large Electron–Positron Collider (LEP) at a depth of about 320 m.w.e. Its hadron calorimeter and scintillator arrays installed at distances up to about 1 km away from ALEPH are used to measure cosmic muon induced time coincidences over large distances. The aim of this experiment (CosmoALEPH) is (1) to study the muon component above 70 GeV of Extensive Air Showers (EAS) and (2) to test the feasibility of searching for time correlations over even larger distances (up to 8 km) between the four LEP detectors. Layout and first results of CosmoALEPH are presented demonstrating the potential for cosmic ray physics in the LEP tunnel. The multiplici…

PhysicsNuclear and High Energy PhysicsAlephParticle physicsAstrophysics and AstronomyCOSMIC cancer databaseMuonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaDetectorCosmic rayParticle detectorlaw.inventionNuclear physicslawHigh Energy Physics::ExperimentColliderInstrumentationLepton
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The read-out processors of the Aleph time projection chamber and their performance

1990

The Aleph detector is installed on the LEP electron-positron storage ring. Its central tracking detector, a time projection chamber (TPC), has about 50000 channels of sampling electronics. The digitized signals are processed by 72 double-width Fastbus modules built around an MC 68020 processor. The time projection processor is described, and the solutions, both hardware and software, adopted to run and manage such a complex system in a Fastbus-VAX environment are discussed. Practical experience with the system is reported. >

PhysicsNuclear and High Energy PhysicsAlephTime projection chamberbusiness.industryDetectorElectrical engineeringTracking (particle physics)Particle detectorSoftwareNuclear Energy and EngineeringNuclear electronicsElectrical and Electronic EngineeringProjection (set theory)businessComputer hardwareIEEE Transactions on Nuclear Science
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